Dielectric relaxation memory
A capacitor structure having a dielectric layer disposed between two conductive electrodes, wherein the dielectric layer contains at least one charge trap site corresponding to a specific energy state. The energy states may be used to distinguish memory states for the capacitor structure, allowing the invention to be used as a memory device. A method of forming the trap cites involves an atomic layer deposition of a material at pre-determined areas in the dielectric layer.
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The present application is a divisional of application Ser. No. 10/930,774, filed Sep. 1, 2004 now U.S. Pat. No. 7,388,248, the entire disclosure of which is incorporated herein by reference.
The present invention relates to the field of memory devices, and in particular to a memory device that utilizes dielectric relaxation.
BACKGROUND OF THE INVENTIONA memory cell in an integrated circuit, such as a dynamic random access memory (DRAM) array, typically comprises a charge storage capacitor (or cell capacitor) coupled to an access device such as a metal oxide semiconductor field effect transistor (MOSFET). The MOSFET functions to apply or remove charge on the capacitor, thus effecting a logical state defined by the stored charge. The amount of charge stored on the capacitor is proportional to the capacitance C, defined by C=kk0A/d, where k is the dielectric constant of the capacitor dielectric, k0 is the vacuum permittivity, A is the electrode surface area and d is the distance between electrodes.
Capacitors, like the capacitors 14 shown in
The current losses from dielectric relaxation are undesirable for many reasons. In DRAM devices, for example, dielectric relaxation can affect the effectiveness of some dielectrics, such as high-k dielectrics, used in the DRAM storage capacitors. In addition, dielectric relaxation can create a threshold shift that severely deteriorates MOSFET performance.
There is a need, therefore, for a memory cell capacitor structure that does not suffer from the undesirable effects of dielectric relaxation but rather can use this phenomenon in a beneficial manner. Accordingly, there is also needed a simple method of producing and operating the desired capacitor structure.
BRIEF SUMMARY OF THE INVENTIONThe present invention provides a capacitor structure having a dielectric layer disposed between two conductive electrodes, wherein the dielectric layer contains at least one charge trap site corresponding to a specific energy state. Energy states may be used to distinguish logical states for the capacitor structure, allowing the invention to be used as a memory device. A method of forming the trap sites involves an atomic layer deposition of a material at pre-determined areas in the capacitor's dielectric layer.
In accordance with an exemplary method of operating the capacitor structure as a memory device, a write voltage is pulsed across the electrodes to fill some or all of the trap sites. The device may be subsequently read using a read voltage applied at the electrodes which senses the filled trap sites as a logical value. In addition, the refresh time may be tuned as desired by adjusting the density and energy state of the trap centers based on the selection of materials.
The foregoing and other advantages and features of the invention will become more apparent from the detailed description of exemplary embodiments provided below with reference to the accompanying drawings in which:
In the following description, reference is made to the accompanying drawings which will serve to illustrate the preferred embodiments of the invention. These embodiments provide sufficient detail to enable those skilled in the art to practice the invention. Of course other embodiments may be used and various changes may be made without departing from the scope of the present invention. The scope of this invention is defined by the appended claims.
Capacitors 100, 100′ formed in accordance with exemplary embodiments of the present invention are shown in cross-sectional view in
In accordance with a first exemplary embodiment of the invention, with reference to
Next, a layer 101 of dielectric material is formed over the bottom electrode 102A. The dielectric material for layer 101 may be, e.g., aluminum oxide, titanium oxide, hafnium oxide, zirconium oxide, or a nitride. Next, a top electrode layer 102B is formed above the dielectric layer 101, and may be formed of any conductive material. Trap sites 104 are then introduced into the dielectric layer 101. This introduction is preferably done by an atomic layer deposition at interstitial sites in the dielectric layer 101. For example, if the dielectric layer 101 is aluminum oxide, it may be doped at pre-determined positions with hafnium, tantalum oxide or hafnium oxide to form charge trap sites 104 within the dielectric matrix 101. High-k materials such as (Ba)TiO3, SrTiO3, PbTiO3, and PbO3 make good trap sites 104, as these materials are known to have significant dielectric relaxation. Potential dopants for creating the trap sites 104 include Hf, Ta, Zr, and Al, which eventually form oxides creating the trap sites 104.
It should be understood that these two embodiments are only exemplary, and that other capacitor structures, like capacitors 100, 100′ are within the scope of the invention, and that trap sites 104, 104′ may be formed as desired. The remaining disclosure applies equally to each exemplary embodiment, and is made with reference to capacitor 100 solely for simplicity purposes.
It is within the scope of the invention that the capacitor 100 may be formed in any known configuration, such as a trench capacitor, a vertical capacitor, a container capacitor, or other capacitor configurations. It should be also be understood that the capacitor 100 may be implemented in a memory device, such as in memory cell 10 as shown in
With reference to
Next, at step 202, a write voltage Vs, larger than the initial voltage V0, is applied to the capacitor dielectric 101 through one of the eletrodes 102A. This higher voltage should cause some or all of the trap sites 104 to fill with charge. With reference to
The second current, Is, should be different than the pre-stress current I0 depending on the trapped charge, meaning the amount of charges in higher energy states. Accordingly, for any given bias condition, the field across the dielectric 101 will be lower or higher depending on the amount of trapped charge. This difference will determine the logical “1” state. Depending on the density and energy state of the trap sites 104, the trapped charge will dissipate during discharge, or return to its original condition, within a given time (e.g., 1 second). Thus, the capacitor 100 needs to be refreshed, at step 204, with application of Vs to the dielectric 101 in order to restore the logical “1” state. The capacitor 100 of the current invention may be tailored to hold a logical “1” state for as long as a flash memory or as short as a DRAM cell.
The above description and drawings are only to be considered illustrative of exemplary embodiments which achieve the features and advantages of the invention. Modification of, and substitutions to, specific process conditions and structures can be made without departing from the spirit and scope of the invention. Accordingly, the invention is not to be considered as being limited by the foregoing description and drawings, but is only limited by the scope of the appended claims.
Claims
1. A method of operating a memory device comprising the acts of:
- applying a first voltage to an electrode of a capacitor structure;
- reading out a current from the capacitor structure;
- applying a second voltage to an electrode of a capacitor structure, wherein the second voltage is greater than the first voltage such that the second voltage causes charge trap sites located within a dielectric layer of the capacitor structure to fill with charge; and
- reading out a second current from the capacitor structure.
2. The method of claim 1, further comprising the act of reapplying the second voltage.
3. The method of claim 1, wherein the act of reapplying the second voltage is performed at pre-determined intervals of time.
4. The method of claim 1, wherein the second voltage is pulsed.
5. The method of claim 4, wherein the second voltage is pulsed, such that the applied voltage returns to the first applied voltage.
6. The method of claim 1, wherein the step of reading out a first and second current comprises reading out a current from the capacitor on an associated bit line.
7. The method of claim 6, further comprising the step of comparing the first current to the second current to determine a memory state of the memory device.
8. A method of operating a memory device comprising the acts of:
- applying a first voltage to a capacitor structure, wherein the first voltage writes a first memory state;
- reading put a first current from the capacitor structure when representing the first memory state;
- applying a second voltage to the capacitor structure, wherein the second voltage causes charge trap sites located within a dielectric layer of the capacitor structure to fill with charge and writes a second memory state; and
- reading out a second current from the capacitor structure when representing the second memory state.
9. The method of claim 8, further comprising the step of comparing the first current to the second current.
10. The method of claim 8, further comprising the step of refreshing the second memory state of the capacitor by reapplying the second voltage.
11. The method of claim 10, wherein the step of reapplying the second voltage is done at pre-determined time intervals.
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Type: Grant
Filed: Mar 27, 2006
Date of Patent: Nov 25, 2008
Patent Publication Number: 20060163633
Assignee: Micron Technology, Inc. (Boise, ID)
Inventors: Cem Basceri (Boise, ID), Gurtej Sandhu (Boise, ID)
Primary Examiner: Ly D Pham
Attorney: Dickstein Shapiro LLP
Application Number: 11/389,150
International Classification: G11C 7/00 (20060101); G11C 11/24 (20060101); G11C 11/34 (20060101); H01L 29/76 (20060101);